English

A critical drift-diffusion equation: intermittent behavior

Probability 2025-11-26 v3 Analysis of PDEs

Abstract

We consider a drift-diffusion process with a time-independent and divergence-free random drift that is of white-noise character. We are interested in the critical case of two space dimensions, where one has to impose a small-scale cut-off for well-posedness, and is interested in the marginally super-diffusive behavior on large scales. In the presence of an (artificial) large-scale cut-off at scale L, as a consequence of standard stochastic homogenization theory, there exist harmonic coordinates with a stationary gradient FLF_L; the merit of these coordinates being that under their lens, the drift-diffusion process turns into a martingale. It has recently been established that the second moments diverge as EFL2lnL\mathbb{E}|F_L|^2\sim\sqrt{\ln L} for LL\uparrow\infty. We quantitatively show that in this limit, and in the regime of small P\'eclet number, FL2/EFL2|F_L|^2/\mathbb{E}|F_L|^2 is not equi-integrable, and that EdetFL/EFL2\mathbb{E}|{\rm det}F_L|/\mathbb{E}|F_L|^2 is small. Hence the Jacobian matrix of the harmonic coordinates is very peaked and non-conformal. We establish this asymptotic behavior by characterizing a proxy F~L\tilde F_L introduced in previous work as the solution of an It\^{o} SDE w. r. t. the variable lnL\ln L, and which implements the concept of a scale-by-scale homogenization based on a variance decomposition and admits an efficient calculus. For this proxy, we establish EF~L4(EF~L2)2\mathbb{E}|\tilde F_L|^4\gg(\mathbb{E}|\tilde F_L|^2)^2 and E(detF~L1)21\mathbb{E}({\rm det}\tilde F_L-1)^2\ll 1. In view of the former property, we assimilate this phenomenon to intermittency. In fact, F~L\tilde F_L behaves like a tensorial stochastic exponential, and as a field can be assimilated to multiplicative Gaussian chaos.

Keywords

Cite

@article{arxiv.2404.13641,
  title  = {A critical drift-diffusion equation: intermittent behavior},
  author = {Felix Otto and Christian Wagner},
  journal= {arXiv preprint arXiv:2404.13641},
  year   = {2025}
}

Comments

Parts of the results of this unpublished preprint are subsumed by the new preprint arXiv:2511.15473

R2 v1 2026-06-28T16:01:12.193Z